|Publication number||US7988297 B2|
|Application number||US 11/875,770|
|Publication date||Aug 2, 2011|
|Filing date||Oct 19, 2007|
|Priority date||Oct 19, 2007|
|Also published as||CA2703721A1, CN101903892A, CN101903892B, EP2247982A2, US20090103052, WO2009052413A2, WO2009052413A3|
|Publication number||11875770, 875770, US 7988297 B2, US 7988297B2, US-B2-7988297, US7988297 B2, US7988297B2|
|Original Assignee||Look Dynamics, Inc.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (74), Non-Patent Citations (4), Referenced by (5), Classifications (53), Legal Events (5)|
|External Links: USPTO, USPTO Assignment, Espacenet|
1. Field of the Invention
This invention relates to optical image processing.
2. State of the Prior Art
There are situations in which useful information can be derived from spatially dispersed portions of light beams. In particular, when an image is being carried or propagated by a light beam, it may be useful to gather and use or analyze information from a particular portion of the image, such as from a particular portion of a cross-section of a beam that is carrying an image. For example, in my U.S. Pat. Nos. 6,678,411 and 7,103,223, which are incorporated herein by reference, narrow, radially oriented portions of a Fourier transform of an image are captured and detected in the spatial domain and used to characterize and encode images by shape for storage, searching, and retrieval. As explained therein, such radially oriented, angularly or rationally spaced portions of light energy from a Fourier transform, i.e., Fourier transform domain, of an image are captured sequentially in the spatial domain, and such portions of the light energy detected in the spatial domain are characteristic of the portions of the image content that are generally linearly aligned in the same angular orientation as the slit in the rotating mask when the light energy is detected. Those systems perform the task of characterizing and encoding images by shape content of the images quite well, but they still have several troublesome shortcomings. For example, the optical systems are quite rigid with little flexibility or tolerance for imperfections in practical optical components or in selection and placement of such components in relation to each other, which results in inherent limitations that constrain the output to less than desirable quality and impose constraints on overall size, optical layout, cost, and packaging.
The accompanying drawings, which are incorporated in and form a part of the specification, illustrate some, but not the only or exclusive, example embodiments and/or features of the present invention. It is intended that the examples and figures disclosed herein are to be considered as illustrative rather than limiting.
In the Drawings:
A system 10 for characterizing, encoding, and storing images by shape content of such images, as illustrated diagrammatically in
The images 12, 14, . . . , n can be in virtually any form, for example, visual images on photographs, films, drawings, graphics, arbitrary patterns, ordered patterns, or the like. They can also be stored and/or generated in or from digital formats or analog formats. Such images can have content that is meaningful in some manner when viewed by humans, or they can appear to be meaningless or not capable of being interpreted by humans but characteristic of some other content, e.g., music, sounds, text, software, and the like. Essentially, any optic pattern of light energy intensities that can be manifested or displayed with discernable shape content can be characterized and encoded with this system 10.
A sample image 12, which can be obtained from any source (e.g., Internet, electronic data base, web site, library, scanner, photograph, film strip, radar image, electronic still or moving video camera, and other sources) is entered into the optical image shape characterizer 10, as will be described in more detail below. Any number n of other sample images 14, . . . , n, are shown in
In the example system 10 illustrated in
As mentioned above, the image 12 can be entered into the optical image characterizer system 10 by the computer 20 and electronically addressable spatial light modulator (E-SLM) 26, which produces a monochromatic version 12′ of the image 12, as will be described in more detail below. The light beam 25 that is incident on the SLM1 26 is also diffracted on a pixel-by-pixel basis. The liquid crystal material in the image-producing SLM1 26 forms a Fourier transform (FT) optic pattern 32, which is unique to the image 12′, at the Fourier transform (FT) plane 33 where the beam 25, 27 is focused to a point 31 by the lenses 30 a and 30 b. Even though it is not recognizable as the image 12′ to the human eye and brain, the complex amplitude distribution of light energy 34 in the optic pattern 32 is the Fourier transform of the complex light distribution in the image 12′, which can be characterized by intensities, i.e., amplitudes, of light energy distributed spatially across the optic pattern 32. Of course, persons skilled in the art will also recognize that an E-SLM is only one of a number of well-known devices, including, but not limited to, optically addressable spatial light modulators, that can create the image 12′ in monochromatic, diffracted light, and this invention is not limited to this particular example.
Concentrations of intense light energy in the Fourier transform (FT) optic pattern 32 at the Fourier transform plane 33 generally correspond to spatial frequencies of the image 12′, i.e., how closely together or far apart features in the image 12′ change or remain the same. In other words, spatial frequencies are also manifested by how closely together or far apart light energy intensities across the light beam 27 change or remain the same. For example, a shirt with a plaid fabric in an image (not shown), i.e., having many small squares, would have a higher spatial frequency, i.e., changes per unit of distance, than a plain, single-color shirt (not shown) in the image. Likewise, portions of an image, such as the bumper and grill parts 35 of the example automobile in image 12′, would have a higher spatial frequency than the side panel 36 portion of the automobile image 12′, because the bumper and grill parts 35 comprise many small pieces with various edges, curves, and other intricate changes within a small spatial distance, whereas the side panel 36 is fairly smooth and uniform over a large spatial distance. Light energy from the finer and sharper details of an image (more spatial frequency), such as the more intricate bumper and grill parts 35 of the image 12′, tend to be dispersed farther radially outward from the optical center or axis 40 in the Fourier transformed image 32 than light energy from more course or plain details of an image (less spatial frequency), such as the side panel 36 of the image 12′. The amplitude of light energy 34 dispersed radially outward in the Fourier transform optic pattern 32 is related to the light energy of the corresponding portions of the optic pattern of image 12′ from which such light energy emanates, except that such light energy is concentrated into areas or bands 34 at the plane 33 of the Fourier transform (FT) optic pattern 32, i.e., into bands of intense light energy separated by bands of little or no light energy, which result from constructive and destructive interference of the diffracted light energy. If the high spatial frequency portions of the image 12′, such as the bumper and grill portion 35, are bright, then the intensity or amplitude of light energy from those high spatial frequency portions of the image 12′, which are dispersed to the more radially outward bands of light energy 34 in the Fourier transform optic pattern 32, will be higher, i.e., brighter. On the other hand, if the high spatial frequency portions of the optic pattern of image 12′ are dim, then the intensity or amplitude of light energy from those high spatial frequency portions of the optic pattern of image 12′, which are dispersed to the more radially outward bands of light energy 34 in the Fourier transform optic pattern 32, will be lower, i.e., not so bright. Likewise, if the low spatial frequency portions of the optic pattern of image 12′, such as the side panel portion 36, are bright, then the intensity or amplitude of light energy from those low spatial frequency portions of the optic pattern of image 12′ which are dispersed by the FT lens to the less radially outward bands of light energy 34 in the Fourier transform optic pattern 32 (i.e., closer to the optical axis 40), will be higher, i.e., brighter. However, if the low spatial frequency portions of the optic pattern of image 12′ are dim, then the intensity or amplitude of light energy from those low spatial frequency portions of the optic pattern of image 12′, which are dispersed by the FT lens 30 to the less radially outward bands of light energy 34 in the Fourier transform optic pattern 32, will be lower, i.e., not so bright.
In summary, the Fourier transform optic pattern 32 of the light emanating from the image 12′: (i) is unique to the image 12′; (ii) comprises areas or bands of light energy 34 concentration, which are dispersed radially from the center or optical axis 40, that represent spatial frequencies, i.e., fineness of details, in the image 12′; (iii) the intensity or amplitudes of light energy 34 at each spatial frequency area or band in the Fourier transform optic pattern 32 corresponds to brightness or intensity of light energy emanating from the respective fine or course features of the image 12′; and (iv) such light energy 34 in the areas or bands of the Fourier transform optic pattern 32 are detectable in intensity and in spatial location by this optical image characterizer system 10.
Since this optical image characterizer system 10 of this invention is designed to characterize an image 12 by shapes that comprise the image 12, additional sectorized spatial filtering of the Fourier transform light energy pattern 32 is used to detect and capture light energy emanating from the finer or sharper details or parts of such finer or sharper details in the image 12′, which are aligned linearly in various specific angular orientations. Such sectorized spatial filtering can be accomplished in any of a number of different ways, as will be explained in more detail below, but an example sectorized spatial filter arrangement for this function is included in a combination of the segmented radial spatial light modulator device (SLM1) 50, which is described in U.S. Pat. No. 7,103,223, together with the polarizer or polarization analyzer 70. Essentially, the segmented radial SLM1 device 50 rotates the plane of polarization of selected sector portions of the Fourier transform optic pattern 32 from p-plane polarization to s-plane polarization, or vice versa, and the polarizer/analyzer 70 separates light energy of those portions of the beam 27 that are isolated and polarized in one plane from the light energy of the rest of the Fourier transform optic pattern 32 that remains polarized in the other plane so that such light energy of the selected and isolated portions can be detected separately at the detector 80, as will be described in more detail below. A rotating mask with a radial slot (not shown), such as that described in U.S. Pat. No. 6,678,411, could also be used for the sectorized spatial filter 50 in the example optical system 800.
In the optical image characterizer 10 illustrated in
The focusing lenses 30 a and 30 b, optional polarizer 28, image-producing SLM1 26, polarizer/analyzer 116, optional polarization rotator 118, and sectorized spatial filter 50 comprise a first overlapping optical subsystem 810 that produces the Fourier transform pattern 32 of the monochromatic image 12′, as will be explained in more detail below. The projecting lenses 78 a and 78 b, polarizer/analyzer 70, and detector 80 comprise a second overlapping optical subsystem 820 that projects the sectorized, spatially filtered, image 60 for detection, as will be described in more detail below. The optional spectral mirror 806 can also be provided to fold the second overlapping optical subsystem 820 into a compact form.
As mentioned above, the focusing lenses 30 a and 30 b are provided to focus the polarized, monochromatic, coherent beam portions 25, 27 to a spot, i.e., focal point 31, on the sectorized spatial filter 50, so that the Fourier transform pattern 32 forms on a Fourier transform plane that contains the focal point 31, but which in one example embodiment is at an angle to the focal plane 33 to prevent feedback that would blur or degrade the Fourier transform pattern and filtered spatial image at the detector 80, as will be explained in more detail below. As also mentioned above, this description will proceed for convenience with the beam portion 25 that is incident on the image-producing SLM1 26 designated as polarized in the s plane, i.e., s-polarized, although it could just as well be p-polarized. The focusing function of lenses 30 a and 30 b could also be accomplished with a single lens or any combination of lenses, as would be apparent to persons skilled in the art, and any such other focusing system that focuses beam portions 25, 27 to a point on the spatial filtering SLM2 is considered to be equivalent. If the optional polarizer 28 is used and positioned between the two focusing lenses 30 a and 30 b, as shown in
As mentioned above, there are many ways of “writing” images 12, 14, . . . , n into a light beam, one of which is with an electronically addressable SLM. In this example, computer 20 has the content of image 12 digitized, so the computer 20 can transmit digital signals via link 21 to the electronically addressable SLM1 26 in a manner that addresses and activates certain pixels in the electronically addressable SLM 26 1 to “write” the image 12′ into reflected light beam 27(p), as is understood by persons skilled in the art. Essentially, the addressed pixels rotate the plane of polarization by 90 degrees from the s-plane of incident beam 25(s) to the p-plane of reflected beam 27(p), or by some lesser amount for gray-scales, in a manner such that the reflected light energy with partially or fully 90-degree polarization plane rotation is in a monochromatic optical pattern of the image 12′. Of course, persons skilled in the art will also understand that the image 12′ could also be created with an electronically addressable SLM that operates in an opposite manner, i.e., the plane of polarization is rotated in reflected light, except where pixels are activated, in which case the computer 20 would be programmed to activate pixels according to a negative of the image 12 in order to write the image 12′ into reflected beam portion 27. Either way, the emerging beam portion 27 of coherent light, carrying image 12′, is p-polarized instead of s-polarized or vice versa. Consequently, in this example, the monochromatic light beam portion 27(p), with its light energy distributed in an optic pattern that forms the monochromatic image 12′, is transmitted by the polarizer/analyzer 116 to the sectorized spatial filter 50 and beyond, instead of being absorbed or reflected by it.
As persons skilled in the art understand, the orientation of the light polarization has to match the imaging SLM1 26 polarization in order for the imaging SLM1 26 to operate effectively. If the optics in the laser source 23 do not provide for adjusting polarization plane adjustment, such matching can be accomplished by rotating the entire laser source 23 about its longitudinal axis, or an optional polarization rotator component, such as a half-wave retarder (not shown) can be positioned in the beam portion 24 or 25 in front of the imaging SLM1 26 and rotated an appropriate amount to achieve the desired polarization plane orientation.
The polarizer/analyzer 116 can be any device that separates p-polarized light from s-polarized light or vice versa. Such devices are well-known and could be, for example, an absorbing polarizer 116, as shown in
As shown in
As mentioned above, the sectorized spatial filter 50 can be a spatial light modulator (SLM2) with pixel groups or other active optical elements that rotate polarization of light in radially extending sectors and/or segments of sectors at selected angular orientations to filter light energy in the Fourier transform pattern 32, as will be described in more detail below. For example, the sectorized spatial filter SLM2 50 depicted in
The second overlapping optical subsystem 820 projects the light energy of the filtered, monochromatic, spatial image 12′ to the detector 80. To do so, the projection lenses 78 a and 78 b are shaped and positioned to project the spatial image 12′ at the SLM1 26 as the object onto the detector 80 as the real image, which requires only that the distance from the object, i.e., image 12′ at SLM1 26, to the detector 80 has to be greater than the focal length of the combination of lenses 78 a and 78 b. Consequently, there is great flexibility in lens parameters, such as size and focal length, and in placement of the projection lenses 78 a and 78 b and detector 80 in relation to each other and in relation to the imaging SLM1 26, spatial filtering SLM2 50, and other components of the first overlapping optical subsystem 810. Such flexibility is useful in many ways. One example is the ability to scale the projected, filtered image to the size of the detector, including, for example, to match pixels or groups of pixels of the image 12′ from the imaging SLM1 26 and/or the filtering SLM2 50 to different sized sensors or groups of sensors in the detector 80.
The polarizer/analyzer 70 separates the p-polarized light in beam portion 61 from the s-polarized light so that only the desired portion of the spatially filtered light from the Fourier transform pattern 32 reaches the detector 80. For example, if the polarizer/analyzer 70 is an absorbing polarizer, as shown in
The concept, structure, and function of the non-rigidly coupled, overlapping optical systems 810, 820 can be illustrated, for example, by
As shown in
The flat SLM1 26 will impose phase changes regardless of the direction of the incident light rays, so the incoming beam 24 does not have to be collimated to form a Fourier transform pattern of the image 12′ at the focal point 31 of the lens 30, as it would have to be if refraction by the lens 30 was being used to form the Fourier transform pattern 32. Therefore, the incoming beam 24 can be diverging from the optical axis 40, as shown in
The SLM1 26 forms the monochromatic image 12′ in the light beam portion 27 by rotating plane of polarization on a pixel-by-pixel basis, so that, for example, the rotated, p-polarized light in beam portion 27 comprises the monochromatic image 12′, and the unrotated, s-polarized light is blocked by the polarizer/analyzer 116. The p-polarized, diffracted light of the image 12′ is transmitted by the polarizer/analyzer 116 so that it interferes and forms the Fourier transform 32 of the image 12′ at the focal plane 33 of the focusing lens 30.
Consequently, the only rigid optical and spatial constraints in the first overlapping subsystem 810 are that the incoming beam 24 has to be monochromatic and coherent light, the lens 30 has to have a focal point 31, the image-producing SLM1 26 has to be positioned somewhere between the focusing lens 30 and the focal point 31 where whatever image 12 it presents is fully illuminated, and the spatial filter 50 has to be positioned where the Fourier transform pattern 32 of the monochromatic image 12′ is presented, i.e., at the focal point 31, or, optionally, at some other projection of the Fourier transform pattern which could be done with another lens (not shown), if desired. In the
Referring again primarily to
Consequently, only the desired portion of the spatial domain image 12′, as selected by the Fourier domain filtering of SLM2 50, gets projected by the projection lens 78 to form the filtered spatial domain image 60 at the detector 80. In other words, the spatial domain image 60 is comprised of only the parts of the spatial domain image 12′ that are selected in the Fourier transform domain. In the example image shape characterizing and encoding application described herein, those parts are the portions of the light rays from the image 12′ that pass through radially extending sectors or segments of sectors in the Fourier transform domain, but they could be any other selected parts filtered in any other way in the Fourier transform domain.
As mentioned above, there is considerable flexibility in component placement. The projection lens 78 has to be between the image producing SLM, 26 and the detector 80 and must have both of its focal points 822, 824 between the image producing SLM1 26 and the detector 80, and the spatial filtering SLM2 50 has to be optically between the image producing SLM1 26 and the projection lens 78. However, those components can be moved or positioned just about anywhere desired within those constraints, depending on practical size and capabilities of the components.
The non-feedback arrangement of the system 800 is shown in more detail in
Because the monochromatic image 12′ is formed by the imaging SLM1 26 in a imaging plane 19 at the angle θ to the axis 40 of the incoming beam portion 25(s), it is also at the same angle θ to the axis 40′ of the reflected beam portion 27, which comprises the image 12′, and the image 12′ is also at the angle α to a plane 816 that is perpendicular to the axis 40′ of beam portion 27. Consequently, the Fourier transform pattern 32 of the image 12′ will form in a plane 818, which includes the focal point 31 on the axis 40′ of the beam portion 27, but which is optically parallel to the imaging plane 19 and at the angle θ to the axis 40′, instead of in the focal plane 33. In other words, the Fourier transform pattern 32 forms in a Fourier transform plane 818, which is at the angle α to the focal plane 33. Therefore, to prevent distortion and to get precise spatial filtering in the plane 818 of the Fourier transform pattern 32, the spatial imaging SLM2 50 is positioned so that its filtering plane is at the focal point 31, but in the plane 818 of the Fourier transform pattern 32, not in the focal plane 33. In other words, the filtering plane of the spatial filtering SLM2 50 is positioned on the focal point 31, but oriented optically parallel to the imaging plane 19 of the imaging SLM1 26, which can be accomplished by positioning the filtering plane physically parallel to the imaging plane 19. If a spectral mirror (not shown) was placed in the beam portion 27, the beam portion 27 could be folded to put the filtering plane 818 of the spatial filtering SLM2 50 so that it is positioned on the focal point 31, but oriented perpendicular to the imaging plane 19 of the imaging SLM1 26, if desired for packaging or other purposes, which would still be effectively optically parallel to the imaging plane 19.
As explained above, the spatial filtering SLM2 50 spatially filters the Fourier transform pattern 32 of the image 12′, and the projection lenses 78 a and 78 b reach back through the spatial filtering SLM2 50 to project the spatial domain image 12′, as filtered by the SLM2 50, onto the detector 80 as the filtered, spatial domain image 60. Therefore, to prevent distortion of the filtered, spatial domain image 60 at the detector 80, the detection plane 826 of the detector 80 also has to be optically parallel to the imaging plane 19 of the imaging SLM1 26. In the
To avoid the “pseudo-p polarization” feedback problem described above, the incident angle α can be any angle that causes the unwanted light to miss the detector. In one example implementation, the incident angle α is chosen to be 13.5° because it provides for a compact system layout with sufficient room for the necessary components and is great enough to “skew” the unwanted reflection far enough to miss the detector 80, as explained above. Such an example layout of the optical image spatial filtering system 800 described above is illustrated in
An example segmented radial spatial light modulator (SLM) device 50 is illustrated diagrammatically in
An enlarged elevation view of the active optic area 54 of the integrated circuit 52 is illustrated in
The selection and isolation of a portion of the incident light beam 27(p) is illustrated in
In the example segmented, radial SLM 50 shown in
Of course, segments in different sectors of different angular orientations about the optical axis 40 will align linearly with features or lines in the image 12′ that have different angular orientations, as will be described in more detail below. Thus, the light energy bands 62 in the filtered pattern 60 will change, as active optic segments in different sectors are selected and activated, to represent different features, details, edges, or lines in the optical pattern of image 12′ at various angular orientations, intricateness or fineness, and brightness, as will be explained in more detail below. In general, however, the light energy bands 62, if inverse Fourier transformed from the FT optic pattern 32 after the above-described spatial filtering 54, will be located in the same spatially-related sites as the features in the original image 12′ from which such light energy emanated. For example, light energy in a band 62 in pattern 60 that originally emanated from bumper and grill parts 35 in image 12′, after spatial filtering with the vertical sector of the bumper and grill parts 35 in image 12′.
The spatially filtered light energy in bands 62 of the filtered pattern 60 can be detected by a photodetector 80 at any of the various angular orientations of the activated sectors and fed electronically to a computer 20 or other microprocessor or computer for processing and encoding. While only one photodetector 80 with an example 16×16 array 82 of individual photosensitive energy transducers 84 is illustrated in
The computer 20, with input of information about the filtered optical patterns 60, i.e., light energy intensity (I) distribution, from the detector array 82, along with information about the image 12 (e.g., identification number, source locator, and the like), information about the angular orientation (R) of the sector in which a segment is activated, and information about the radial distance or scale (S) of the activated segment relating to spatial frequency, can be programmed to encode the characteristics of the image 12 relating to the shape content of the image 12. One useful format for encoding such information is by pixel of the filtered image 60, including information regarding x, y coordinate location of each pixel, Rotation (i.e., angular orientation of the sector in which a segment is activated, thus of the linear features of the image 12 that align with such angular orientation), and Intensity (i.e., amplitude of light energy from the filtered pattern 60 that is detected at each pixel at the angular orientation R. A searchable flag, such as a distortion factor X, can also be provided, as explained, for example, in U.S. Pat. No. 6,678,411, or by a ghost image pre-processing feature as explained, for example, in U.S. Pat. No. 7,103,223. Such combination of angular orientation or rotation R, light energy intensity I for each pixel, and distortion factor X can be called a “RIXel” for short. Scale (i.e., spatial frequencies of image 12 content at such angular orientations) can also be included in such encoding, if desired. When including a scale factor S, the combination can be called a “RIXSel”. Each RIXel or RIXSel can then be associated with some identifier for the image 12 from which it was derived (e.g., a number, name, or the like), the source location of the image 12 (e.g., Internet URL, data base file, book title, owner of the image 12, and the like), and any other desired information about the image, such as format, resolution, color, texture, content description, search category, or the like. Some of such other information, such as color, texture, content description, and/or search category, can be information input from another data base, from human input, or even from another optical characterizer that automatically characterizes the same image 12 as to color, texture, or the like-whatever would be useful for searching, finding, or retrieving image 12 or for comparing image 12 to other images.
Some, all, or additional combinations of such information about each image 12, 14 . . . , n characterized for shape and encoded, as described above, can be sent by the computer 20 to one or more data base(s) 102. Several example data base architectures 104, 106, 108 for storing RIXel or RIXSel information about each image 12, 14, . . . , n are shown in
The Fourier transform optic pattern 32, as mentioned above, is symmetrical from top to bottom and from left to right, so that each semicircle of the Fourier transform optic pattern 32 contains exactly the same distribution and intensity of light energy as its opposite semicircle. Light energy from lower spatial frequencies in the image 12′ are distributed toward the center or optical axis 40′ of the Fourier transform optic pattern 32, while the light energy from higher spatial frequencies in the image 12′ are distributed farther away from the optical axis 40′ and toward the outer edge of the pattern 32, i.e., farther radially outward from the optical axis 40′. Light energy from features in the image 12′ that are distributed vertically in the image 12′ to create those various spatial frequencies is likewise distributed vertically in the Fourier transform optic pattern 32. At the same time, light energy from features in the image 12′ that are distributed horizontally in the image 12′ to create those various spatial frequencies is distributed horizontally in the Fourier transform optic pattern 32. Therefore, in general, light energy from features in the image 12′ that are distributed in any angular orientation with respect to the optical axis 40′ to create the various spatial frequencies in the image 12′ is also distributed at those same angular orientations in the Fourier transform optic pattern 32. Consequently, by detecting only light energy distributed at particular angular orientations with respect to the optical axis 40′ in the Fourier transform optic pattern 32, such detections are characteristic of features or details in the image 12′ that are aligned linearly in such particular angular orientations. The radial distributions of such detected light energy at each such angular orientation indicate the intricateness or sharpness of such linear features or details in the image 12′, i.e., spatial frequency, while the intensities of such detected light energy indicate the brightness of such features or details in the image 12′.
Therefore, a composite of light energy detections at all angular orientations in the Fourier transform optic pattern 32 creates a composite record of the shapes, i.e., angular orientations, intricateness or sharpness, and brightness, of linear features that comprise the image 12′. However, for most practical needs, such as for encoding shape characteristics of images 12, 14, . . . , n for data base storing, searching, retrieval, comparison and matching to other images, and the like, it is not necessary to record such light energy detections for all angular orientations in the Fourier transform pattern 12′. It is usually sufficient to detect and record such light energy distributions and intensities for just some of the angular orientations in the Fourier transform optic pattern 32 to get enough shape characterization to be practically unique to each image 12, 14, . . . , n for data base storage, searching, and retrieval of such specific images 12, 14, . . . , n. For purposes of explanation, but not for limitation, use of 11.25-degree angular increments is convenient and practical, because there are sixteen (16) 11.25-degree increments in 180 degrees of rotation, which is sufficient characterization for most purposes and has data processing and data storage efficiencies, as explained in U.S. Pat. No. 6,678,411. However, other discrete angular increments could also be used, including constant increments or varying increments. Of course, varying increments would require more computer capacity and more complex software to handle the data processing, storing, and searching functions.
The segmented radial SLM 50, shown in
The preferred, but not essential, shape of the active optic sectors, e.g., sector 500, in the segmented radial SLM 50 is a narrow, elongated wedge. The width of the wedge will depend on the light energy available or needed and the optic resolution desired. A wider sector will direct more light energy 34 to the detector 80, but precision of line or feature resolution of the image 12′ will degrade slightly. A narrower sector will get better line resolution, but with a corresponding increase in the complexity of the resulting pattern shape generalization and complexity and a decrease in light energy directed to the detector 80. There may also be a practical limitation as to how narrow and close the wedges can be made with the connecting electric traces in a limited active optic area 54 in an economic and efficient manner. Therefore, a desirable balance between these resolution, detectability, and size considerations may be struck in choosing sector size. Also, for specialized applications, sectors of different shapes (not shown), such as ovals, or other shapes could be used to capture shapes other than lines from the image 12.
The number of active optic segments in a sector, e.g., the four segments 502, 504, 506, 508 in sector 500, also has similar constraints. Smaller segments direct less light energy to the detector 80, but may provide more resolution of shape characteristics of the image 12′, whereas larger segments direct more light to the detector 80, thus are more easily detectable, but resolution decreases. For lower resolution applications or requirements, the sectors may not even need to be divided into segments, and this invention includes radial spatial light modulators in which each sector 500, 510, 520, 530, 540, 550, 560, 570, 580, 590, 600, 610, 620, 630, 640, 650 is not segmented, thus comprises a single active optic element for each sector. However, the same lower resolution effect can be achieved in the illustrated embodiment 50 in
In this example embodiment of SLM2 50, each sector, e.g., sector 500, comprises four individually addressable, active optic segments, e.g., segments 502, 504, 506, 508, as shown in
To illustrate, suppose the image 12′ is a pattern of a plurality of parallel vertical lines intersecting a plurality of parallel horizontal lines to form a matrix of squares, as illustrated, for example, in
Also, light energy for the horizontal shape content of such large, small, or intermediate sized matrix square patterns would be incident on the respective inner, outer, or intermediate positioned segments of the horizontal sector 540. For example, in the image 12′ of
Further, any features of an image 12′ that have sizes over 50 percent of the size of image 12′, which light energy is incident on the center area portion 41, can either be captured and detected as an indicator of general brightness of the image 12′ for intensity control or calibration purposes or just ignored and not captured or detected at all, because there is little, if any, useable shape information or content in the light energy that comprises that 50 percent of the size of the image 12′. Likewise, the approximately 3⅛ percent of the size content of the image 12′ that is radially outward beyond the outer segments or sectors is not detected and can be ignored in this preferred configuration. The center 41 can be made optically active to capture light energy incident thereon, if it is desired to capture and detect such light energy for general brightness indication, intensity control, or calibration purposes, as will be understood and within the capabilities of persons skilled in the art. For example, if an image 12′ has a matrix of squares, which are so large that the distance between the vertical lines, which define the edges of the large squares, is over 50 percent of the width of the image 12′, there is little, if any, vertical shape content of practical use, and the light energy for that vertical shape content is incident on the center area portion 41. On the opposite end of the spectrum, if such an image 12′ has a matrix of squares, which are so small that the distance between the vertical lines, which define the edges of the small squares, is less than about 3⅛ percent of the width of the image 12′, there is also little, if any, vertical shape content of practical use, and the light energy for such vertical shape content is dispersed radially outward, beyond the outer segment 508 of sector 500. Of course, other configurations or scale segment sizes and combinations of the segmented radial SLM 50 could also be made and used within the scope of this invention.
The shape content detection will be described in more detail below by use of the example automobile image 12′ of
On the other hand, if the image 12′ has a matrix of very small squares 722, thus high spatial frequency, as shown in
In summary, for an image 12′ comprising a matrix of squares, as described above, actuation of the inner segment 502 of vertical sector 500 and getting vertical lines formed in the spatial domain, while actuation of the outer segment 508 as well as the intermediate segments 504, 506, in the vertical sector 500 projects no vertical lines in the spatial domain, would show that the vertical shape content of the image has low spatial frequency characteristic of large squares 702 in
If analysis of other non-vertical and non-horizontal sectors 510, 520, 530, 550, 560, 580, 590, 600, 610, 620, 630, 640, 650 show no lines in the spatial domain from those angular orientations, then the recordable results confirm the shape content of the image 12′ to be only a smaller or larger spatial frequency at some or all of those angular orientations, then the recordable results would confirm some shape complexity in addition to the matrix of squares in the image 12′. Thus, shape information, including spatial frequency or scale (S), and intensity (I) at each angular orientation or rotation (R) can be acquired with the spatial light modulator 50 in the system of this invention.
In summary, for an image 12′ with the large square 702 matrix shown in
As illustrated in
A transparent conductive layer 190 deposited on the front substrate 182 is connected by another lead 513 to another voltage V3. Therefore, a voltage can be applied across the portion of the liquid crystal material 180 that is sandwiched between the metal layer 186 and the transparent conductive layer 190 by, for example, making V1 positive and V3 negative and vice versa. Likewise, when a voltage can be applied across the portion of the liquid crystal material 180 that is sandwiched between the metal layer 188 and the transparent conductive layer 190 by, for example, making V2 positive and V3 negative and vice versa.
As mentioned above, the function of the respective segments 506, 508 is to rotate the plane of polarization of selective portions of the incident light beam 27(p) so that those portions of the light beam 27(p), which carry corresponding portions of the Fourier transform optic pattern 32, can be separated and isolated from the remainder of the light beam 27(p) for detection by the photodetector array 82 (
One example system, but certainly not the only one, can use a liquid crystal material 180 that transmits light 27(p) without affecting polarization when there is a sufficient voltage across the liquid crystal material 180 and to act as a ¼-wave retarder when there is no voltage across the liquid crystal material. An untwisted crystal material 180 that is birefringent in its untwisted state can function in this manner. Thus, for example, when no voltage is applied across the liquid crystal material 180 in segment 508, there is no molecular rotation of the liquid crystal material 180 in outer segment 508, and the liquid crystal material in outer segment 108, with the proper thickness according to the liquid crystal manufacturer's specifications, will function as a ¼-wave plate to convert p-polarized light 27(p) incident on outer segment 508 to circular polarization as the light passes through the untwisted liquid crystal material 180. Upon reaching the metal layer 188, which is reflective, the light is reflected and passes back through the liquid crystal material to undergo another ¼-wave retardation to convert the circular polarization to linear polarization, but in the s-plane, which is orthogonal to the p-plane. The reflected light 61(s), therefore, has its plane of polarization effectively rotated by 90 degrees in relation to the incident light 27(p).
Meanwhile, if there is a sufficient voltage on, for example, the near outer segment 506, to rotate the long axes of the liquid crystal molecules into alignment with the direction of propagation of the incident light waves 27(p), thereby eliminating the birefringence of the liquid crystal material 180, then there is no change of the linear polarization of the light on either its first pass through the liquid crystal material 180 or on its second pass through the liquid crystal material after being reflected by metal layer 186. Consequently, under this condition with a voltage applied across the liquid material 180 in near outer segment 506, the reflected light 61(p) is still polarized in the p-plane, i.e., the same plane as the incident light 27(p).
Many liquid crystal materials require an average DC voltage bias of zero, which can be provided by driving the voltage V3 with a square wave function of alternating positive and negative voltages for equal times. Therefore, for no voltage across the liquid crystal material 180, the other voltages V1, V2, etc., can be driven in phase with equal voltages as V3. However, to apply a voltage across the liquid crystal material 180 adjacent a particular metal layer 186, 188, etc., to activate that particular segment 506, 508, etc., as described above, the respective voltage V1 or V2, etc., can be driven out of phase with V3. If the frequency of the square wave function is coordinated with the switching speed of the liquid crystal material 180, one-half cycle out of phase for a voltage V1, V2, etc., will be enough to activate the liquid crystal material 180 to rotate the plane of polarization of the light as described above.
As mentioned above, other alternate arrangements and known liquid crystal materials can reverse the results from an applied voltage. For example, a twisted liquid crystal material 180 may be used to rotate plane of polarization under a voltage and to not affect plane of polarization when there is no voltage.
Referring again primarily to
Instead, the s-polarized light 61(s) is reflected by the mirror 806 to the detector 80 in the spatial domain. The lens 78 projects the filtered image 12′ via the isolated beam 61(s) in a desired size in the spatial domain on the detector array 82 of photodetector 80.
The photodetector array 82, as mentioned above, can be a 16×16 array of individual light sensors 84, such as charge coupled devices (CCDs), as shown in
The spatial filtering process described above and its characterization of the image 12 by shape content is illustrated in more detail in
This principle also facilitates design and fabrication of an effective spatial filtering SLM2 50, because, for every active optic sector, there can be an adjacent inactive sector or area available for placement of electrically conductive traces to the segments, as shown by reference back to
Returning now to
For example, shape content in the light energy characteristic of that incident on both the vertical 11.25° sector 500 centered at 0° as well as on the non-active area 581 centered at 180° can be detected by effectively activating the active optical segments 502, 504, 506, 508 of sector 500. Shape content in the light energy characteristic of that incident on the 11.25° sector 590 centered at 191.25° as well as on the non-active area 501 centered at 11.25° can be detected effectively by activating the active optic segments of sector 590, because the active optic sector 590 is centered diametrically opposite the non-active area of 11.25°. Shape content in the light energy characteristic of that incident on either the 11.25° sector 510 centered at 22.5° or the non-active area 591 centered at 202.5° can be detected by activating the active optic segments of sector 510. Shape content in the light energy characteristic of that incident on either the 11.25° non-active area centered at 33.75° or active sector 600 centered at 213.75° can be detected by activating the active optic segments of sector 600, which is centered diametrically opposite 33.75° at 213.75°. Shape content in the light energy characteristic of that incident on either the 11.25° sector 520 centered at 45° or non-active area 601 centered at 225° can be detected by activating the active optic segments of sector 520. Shape content in the light energy characteristic of that incident on either the 11.25° non-active area 521 centered at 56.25° or the active sector 610 centered at 236.25° can be detected by activating the active optic segments of sector 610, which is centered diametrically opposite 56.25° at 256.25°. Shape content in the light energy characteristic of that incident on either the 11.25° sector 530 centered at 67.5° or the non-active area 611 centered at 247.5° can be detected by activating the active optic segments of sector 530. Shape content in the light energy characteristic of that incident on either the 11.25° non-active area 531 centered at 78.75° or active sector 620 centered at 258.75° can be detected by activating the active optic segments of sector 620, which is centered diametrically opposite 78.75° at 258.75°. Shape content in the light energy characteristic of that incident on either the 11.25° sector 540 centered at 90° or non-active area 621 centered at 270° can be detected by activating the active optic segments of sector 540. Shape content in the light energy characteristic of that incident on either the 11.25° non-active area 541 centered at 101.25° or the active sector 630 centered at 281.25° can be detected by activating the active optic segments of sector 630, which is centered diametrically opposite 101.25° at 281.25°. Shape content in the light energy characteristic of that incident on either the 11.25° sector 550 centered at 112.5° the diametrically opposite portion of non-active area 631 that is centered at 292.5° can be detected by activating the active optic segments of sector 550. Shape content in the light energy characteristic of that incident on the 11.25° sector 560 centered at 123.75°. The diametrically opposite portion of non-active area 631 that is centered at 303.75° can be detected by activating the active optic segments of sector 560. Shape content in the light energy characteristic of that incident on the 11.25° non-active area 561 centered at 135° or active sector 640 centered at 315° can be detected by activating the active optic segments of sector 640, which is centered diametrically opposite 135° at 315°. Shape content in the light energy characteristic of that incident on the 11.25° sector 570 centered at 146.25° or non-active area 641 centered at 326.25° can be detected by activating the active optic segments of sector 570. Shape content in the light energy characteristic of that incident on the 11.25° non-active area 571 centered at 157.5° or active sector 650 centered at 337.5° can be detected by activating the active optic segments of sector 650, which is centered diametrically opposite 157.5° at 337.5°. Finally, shape content in the light energy characteristic of that incident on the 11.25° sectors 580 centered at 168.75° or non-active area 651 centered at 348.75° can be detected by activating the active optic segments of sector 580.
While it would be unnecessarily cumbersome to illustrate and describe the shape detecting and characterizing functionality of all the active optic segments of all the sectors 500, 510, 520, 530, 540, 550, 560, 570, 580, 590, 600, 610, 620, 630, 640, 650, it may be helpful to illustrate and describe the functionality and results of activating several representative examples of the active optic segments in the active optic area 54. Therefore,
The light energy bands 34, when reflected by the activated outer segment 508, are filtered through the polarizing beam splitter 70 and projected in the filtered optic pattern 60, which is comprised primary of vertical lines or bands 62 of light energy illustrated diagrammatically in
To illustrate further, the near inner segment 504 of active optic sector 500 is shown in
Another example angular orientation of light energy 34 from the FT optic pattern 32 is illustrated by
Capture and detection of horizontal portions of lines, edges, and features 68, 68′ of the image 12′ of respective spatial frequencies, if present in the image 12′, is accomplished by activation of one or more segments 542, 544, 546, 548 of horizontal sector 540, which is oriented 90° from the vertical 0°. The portion of the light energy 34 that is reflected by each activated segments 542, 544, 546, 548 of the horizontal sector 540 is characteristic of all of the substantially horizontal features, parts, and lines 68 of the respective spatial frequencies in the image 12′ that correspond to the light energy, if any, that is incident on those segments in the FT plane 32, as shown in
One more example activated segment 598 in sector 590, is illustrated in
Referring again to
It should be clear by now that any particular angular orientation R of segments of sectors in the active optic area 54 will allow detection of all the shape characteristics of image 12′ that have substantially that same angular orientation R. It should also be clear that radial outward spacing or scale (S) of the segments relates to spatial frequency of such shape characteristics. Thus, all of the shape characteristics of the image 12′ can be detected by detecting the bands 62 of the respective filtered patterns 60 with the segments at all angular orientations. However, as mentioned above, it is sufficient for most purposes to detect some, preferably most, but not necessarily all, of the shape characteristics of the image 12′ by choosing to detect the light energy bands 34 of filtered patterns 60 at certain selected increments of angular orientation or rotation R. Obviously, the bigger the increments of angular orientation of the sectors where light energy bands 34 are detected, the less precise the detected shape characteristics or contents of the image 12′ will be. On the other hand, the smaller the increments of angular orientation, the more data that will have to be processed. Therefore, when selecting the angular increments of sectors at which light energy bands 34 will be detected and recorded, it may be desirable to strike some balance between preciseness of shape characteristics needed or wanted and the speed and efficiency of data processing and storage required to handle such preciseness. For example, but not for limitation, it is believed that detection and recording of the shape characteristics at angular increments of in a range of about 5 to 20 degrees, preferably about 11.25-degrees, will be adequate for most purposes. Also, the angular area of detection can be varied. For example, even if active optic sectors are oriented to detect shape characteristics at angular increments of 11.25°, the active optic areas could be narrow, such as in a range of 3° to 8°, more or less, which would filter out some of the optic energy from the FT optic pattern 32 between the sectors. However, such loss of light energy from non-active areas between sectors or other radially extending sensors, as described elsewhere in this specification, may not be detrimental to shape characterization by this invention, depending on specific applications of the technology to particular problems or goals.
Instead of the radially extending, wedge-shaped active optic sectors and segments of sectors described above, an alternate configuration can be comprised of radially extending, rectangular-shaped active optic modulators as illustrated diagrammatically in
Another, albeit less efficient embodiment, is illustrated in
While the reflective spatial light modulator structure described above in connection with the cross-sectional view of
In the description above, the shape content of a desired angular orientation (R) and scale (S) of an image is captured by masking or blocking all other light in the FT plane 32 from reaching the detector 80 so that only the light energy from that angular orientation (R) and scale segment of the FT plane 32 gets projected back into the spatial domain for detection. However, persons skilled in the art will recognize that shape characterization and encoding with the components described above can also be practiced in the negative. In other words, instead of actuating the one or several segments and/or sectors to get shape content relevant to the angular orientation or rotation (R) and/or radial distance (S) of particular sectors and/or segments, as described above, it would also be feasible to actuate all of the other sectors and segments in the active optic area 54 and not actuate the specific sector and/or segments in order to get a negative or inverse of the shape content of the image. This procedure can be repeated for all of the desired angular (R) and/or scalar (S) sectors and segments so that the composite of information regarding light energy distribution collected and recorded represents a negative or inverse of all of the shape content of an image 12′.
For example, referring back to
To explain further, a negative of the spatially filtered image 60 of the automobile illustrated in
Again, as with the positive spatial images of the shape content, such negative or inverse spatial images can be detected at 80 (
While a number of example implementations, aspects, and embodiments have been described above, persons skilled in the art will recognize other modifications, permutations, additions, and subcombinations that are within the scope and spirit of the claimed invention. Therefore, it is intended that the following claims and claims hereafter introduced are interpreted and construed to include all such modifications, additions, and subcombinations and equivalents as are within their true spirit and scope, and to not limit such claims the exact construction and process shown and described above. The words “comprise,” “comprises,” “comprising,” “composed,” “composes,” “composing,” “include,” “including,” and “includes” when used in this specification and in the following claims are intended to specify the presence of stated features, integers, components, or steps, but they do not preclude the presence or addition of one or more other features, integers, components, steps, or groups thereof.
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|U.S. Classification||353/20, 359/372, 382/280, 359/11, 359/27, 382/199, 382/210, 372/99, 382/106, 359/371, 359/383, 382/140, 250/337, 382/189, 382/211, 353/34, 382/203, 382/127, 359/386, 353/98, 382/146, 382/151, 353/30, 353/122, 382/250, 250/311, 382/168, 382/266, 382/152, 382/248, 382/260, 359/35, 359/1, 372/50.11, 359/13, 359/19, 359/237, 353/69, 382/274, 382/278, 372/103, 353/25, 372/22, 382/177, 353/38, 359/397, 359/385, 250/397, 372/50.124|
|Cooperative Classification||G06K2009/585, G06K9/58|
|Dec 10, 2007||AS||Assignment|
Owner name: LOOK DYNAMICS, INC., COLORADO
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:CRILL, RIKK, MR.;REEL/FRAME:020223/0607
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|Jan 7, 2008||AS||Assignment|
Owner name: LOOK DYNAMICS, INC., COLORADO
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:CRILL, RIKK, MR;REEL/FRAME:020327/0903
Effective date: 20071204
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